lhc first lhc emittance measurements at 6.5 tev ibic15 melbourne, australia 2015 maria kuhn 1,2 –...
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LHC
First LHC Emittance Measurements at 6.5 TeV
IBIC15 Melbourne, Australia 2015
Maria Kuhn1,2 – September 16, 2015
F. Antoniou2, E. Bravin2, B. Dehning2, J. Emery2, V. Kain2, A. Langner1,2, Y. Papaphilippou2, E. Piselli2, G. Trad2
,
1Hamburg University, Hamburg, Germany,2CERN, Geneva, Switzerland
LHC
M. Kuhn - Sept. 16, 2015
Introduction: LHC Cycle and Beam Parameters
o Injection
o Ramp
o Squeeze
o Collisions
2
450 GeV injection plateau (30min)
Energy ramp (20.2 min)
b* squeeze (12.5 min)
o Two circulating beams.
− Beam 1 rotating clockwise, beam 2 counter-clockwise.
o Collisions in four interaction points in the LHC.
− ATLAS and CMS are the two large multi purpose detectors.
LHC
M. Kuhn - Sept. 16, 2015
Introduction: LHC Cycle and Beam Parameters
o Injection
o Ramp
o Squeeze
o Collisions
3
450 GeV injection plateau (30min)
Energy ramp (20.2 min)
b* squeeze (12.5 min)
Proton beam parameters LHC Design 2012 LHC Early 2015 LHC
# bunches/ beam 2808 1374 3 - 458Bunch spacing [ns] 25 50 25 and 50Mean bunch length [ns] 1.3 1.2 1.2Bunch intensity [1011 p] 1.15 1.1 - 1.7 1.0 – 1.2Emittance at injection [mm] 3.5 1.5 – 2.0 1.5 – 3.0Collision energy/beam [TeV] 7 4 6.5Emittance at collision [mm] 3.75 2.4 1.5 – 4.0b* at ATLAS/CMS [m] 0.55 0.6 0.8
LHC
M. Kuhn - Sept. 16, 2015
o In 2012 LHC was operated with high brightness beams.
− Transverse emittance could not be preserved during the LHC cycle.
− ~ 0.4 – 0.9 mm normalized emittance growth from LHC injection to start of collisions.
− But emittance measurement precision during LHC Run 1 doubtful.
Reminder: 2012 Emittance Blow-up
4
2012 LHC performance
LHC
M. Kuhn - Sept. 16, 2015
LHC Wire Scanner Intensity Limitations
o Several types of beam profile measurement systems in the LHC.
− The wire scanners are the most precise and versatile instruments.
− Two operational wire scanners per beam.
• Horizontal and vertical.
o Wire scanners cannot be used with high intensity physics fills.
− Synchrotron light telescope (BSRT) is used for that purpose.
o BSRT cross calibrated with wire scanners.
o Currently, wire scanners are the only instrument to measure beam sizes through the LHC energy ramp.
− Low intensity test fills (a few bunches) are measured to evaluate emittance preservation during the LHC cycle.
5
LHC
M. Kuhn - Sept. 16, 2015
Run 2 LHC Wire Scanner Accuracy
o Transverse normalized emittance e:
− (For location with no dispersion)
LHC Run 2 optics measured with k-modulation at 450 GeV and turn-by-turn phase advance method at 6.5 TeV.
− b function accuracy better than 3 %.
6
𝜺𝒙 ,𝒚=𝜸𝝈 𝒙 , 𝒚
𝟐
𝜷𝒙 ,𝒚
Wire scanner beam size s accuracy
− Wire position measurement precision
• Estimated position measurement potentiometer precision: 50 mm
− Wire position measurement calibration
• Verified with beam by orbit bump scans at the wire scanner location
Lorentz factor g (beam
energy)
LHC
M. Kuhn - Sept. 16, 2015
Wire Position Measurement Calibration
o Using local orbit bumps to verify the wire position measurement calibration of the wire scanners.
− Beam position measured with LHC orbit system and extrapolated to wire scanner.
− Compared to mean position obtained from Gaussian fit to measured transverse beam profile.
− Measurements at 450 GeV and 6.5 TeV are consistent.
Overestimating B2V emittances by 6.6 %.
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Example B2V1: slope of linear fit shows + 3.3 % calibration
error.
LHC
M. Kuhn - Sept. 16, 2015
Wire Scanner Emittance Measurement Errors
o Wire scanner position calibration verification results (Decalibration):
− Another set of orbit bumps foreseen for the near future to check reproducibility of obtained results.
− The results in this talk do not include a correction of the calibration.
o All wire scanner measurements show large s spread from scan to scan (De450GeV and De6.5TeV).
− Depending on scanner and energy.
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Wire Scanner Decalibration [%]De450GeV [%]
De6.5TeV [%]
B1H2 + 7.2 25 20B1V2 - 5.2 20 10B2H1 + 9.0 25 15B2V1 + 6.6 15 10
LHC
M. Kuhn - Sept. 16, 2015
Photomultiplier Working Point Investigations
o Wire scanner shower product amplified by photomultiplier (PM).
− Amplification settings (gain + filter) can alter obtained beam profile.
o LHC Run 1: strong dependence of measured s on PM settings.o Optimum PM working point has to be established!
− Scan through all available gain and filter setting combinations.
9
Bunches with different beam sizes were injected.
To remove natural e growth, scans with fixed reference settings done after each settings change.
Exponential fit
Example: B2V1 at 450 GeV
LHC
M. Kuhn - Sept. 16, 2015
Photomultiplier Working Point Investigations
o Wire scanner shower product amplified by photomultiplier (PM).
− Amplification settings (gain + filter) can alter obtained beam profile.
o LHC Run 1: strong dependence of PM settings on measured .s
o Optimum PM working point has to be established!
− Scan through all available gain and filter setting combinations.
10
Measured beam sizes minus the fitted growth.
Measurements with same gain + filter settings are averaged.
No sign of PM saturation at 450 GeV could be detected.
Same for 6.5 TeV.
LHC
M. Kuhn - Sept. 16, 2015
First Emittance Measurements (1)
o Example Fill 4284 (August 28, 2015):
− 3 bunches with different initial emittances, intensities (0.6 – 1.1 x 1011 ppb) and bunch lengths (1.0 – 1.25 ns).
11
IBS simulations with MADX IBS module include measured initial beam parameters, dispersion, and radiation damping.
Measurements in the horizontal planes match IBS simulation.
LHC
M. Kuhn - Sept. 16, 2015
First Emittance Measurements (2)
o Example Fill 4284 (August 28, 2015):
− 3 bunches with different initial emittances, intensities (0.6 – 1.1 x 1011 ppb) and bunch lengths (1.0 – 1.25 ns).
12
IBS simulations with MADX IBS module include measured initial beam parameters, dispersion, and radiation damping.
Measurements in the horizontal planes match IBS simulation.
e450GeV [mm]
e6.5TeV
[mm]De [%] Desim [%]
B1H 1.90 2.08 9 8B1V 1.71 2.04 19 -2B2H 1.50 1.65 10 10B2V 1.58 1.95 23 -2
Emittance growth through the cycle of bunch 3
Vertical emittance growth through the cycle could not be reproduced with IBS simulations.
LHC
M. Kuhn - Sept. 16, 2015
Emittance Growth during the LHC Ramp
o Measured b during ramp not yet available.
− Using linear interpolation of measured b at injection + flattop.
o Current b knowledge results in unphysically growing/shrinking e.
− Run 1 experience: non-monotonically changing b functions during the ramp.
13
Measurements in the horizontal planes consistent with IBS simulations during the ramp.
Beam 2 vertical emittances grow 20 % (~ 0.3 mm).
LHC
M. Kuhn - Sept. 16, 2015
Emittance Preservation during the Squeeze
o Within measurement accuracy emittances are conserved during the b* squeeze.
− Result is reproducible.
14
Emittances measured with BSRT and averaged over several hundred measurements.
Also need measured b functions during the squeeze.
LHC
M. Kuhn - Sept. 16, 2015
Emittance at Start of Collisionso Comparison of emittance from wire scans
and luminosity:
− Fill 3954 (July 4, 2015), one bunch in collision.
− According to experts ATLAS luminosity low by ~10 % with uncertainty±10 %.
• 5 % error on crossing angle
• ±1 cm error on measured bunch length.
• b* measured with k-modulation with 1 % uncertainty.
o Preliminary: ATLAS and wire scanner results agree within errors.
− Better than during Run 1.
15
Injection Collision GrowthWS e [mm] 2.51 ± 0.10 2.75 ± 0.20 0.24 10 %ATLAS e [mm] n.a. 2.97 ± 0.36 0.46 19 %
L …. Luminosityk …. # bunchesN …. # protons / bunchf …. Revolution freq.F …. Luminosity reduction factor
𝐿=𝑘𝑁 2 𝑓 𝛾4 𝜋 𝛽∗𝜀
∙𝐹
LHC
M. Kuhn - Sept. 16, 2015
Radiation Damping at 6.5 TeVo At high energies protons circulating in the LHC emit enough
synchrotron radiation to modify the beam parameters
− First observed during LHC Run 2
− Counteracts IBS: reduction of vertical emittance
16
Simulations with MADX IBS module.
Simulation predicts slightly faster emittance decrease than measured with BSRT.
Additional emittance growth from proton collisions + beam–beam effects not included in the simulation.
LHC
M. Kuhn - Sept. 16, 2015
Current Performance of the LHCo Emittance in collisions
derived from luminosity.
o Injection emittance of first batch measured with SPS and LHC wire scanners.
Emittance blow-up through the cycle:
o 50 ns beams show very little blow-up (~ 10 %), much smaller than during Run 1.
o Large blow-up for 25 ns beams (25 % for most recent fills).
− Electron cloud effects
− Beam instabilities
17
LHC
M. Kuhn - Sept. 16, 2015
Summary & Conclusiono Good progress in understanding wire scanner emittance
measurements for LHC Run 2.
− Wire scanner calibration verified, no PM saturation effects detected.
Emittance growth during the LHC cycle:
− Horizontal emittance growth matches IBS simulations.
− Small growth in the vertical planes not yet understood.
• Caveat: single bunch fills.
− Synchrotron radiation damping observed for the first time at 6.5 TeV.
− With still not fully calibrated luminosity data: emittances from wire scans and ATLAS luminosity agree within errors.
o Smaller emittance blow-up (~ 10 %) through the cycle than during Run 1 for 50 ns beams.
o 25 ns physics beams show much larger growth.
− Electron cloud effects and beam instabilities. 18
LHC
M. Kuhn - Sept. 16, 2015
Outlineo LHC cycle and beam parameters
− LHC Run 1 transverse normalized emittance blow-up
o LHC wire scanner intensity limitations
o Run 2 LHC wire scanner accuracy
− Wire position measurement calibration
− Photomultiplier working point investigations
o First transverse normalized emittance measurements
− Emittance growth during the LHC ramp
− Emittance preservation during the squeeze
− Emittance at start of collisions
− Radiation damping at 6.5 TeV
o Current performance of the LHC
20
LHC
M. Kuhn - Sept. 16, 2015
CERN Accelerator Complex
21
Beam 1
TI2
Beam 2
TI8
LHC proton path
The LHC needs most of the CERN accelerators...
LHC
M. Kuhn - Sept. 16, 2015
Photomultiplier Saturation Studies Run 1
o Photomultiplier (PM) gain and filter can have a strong influence on measured beam size
− See measurements of 2012
22
PM saturation studies at 4 TeV in 2012.
PM saturation studies at 450 GeV in 2012.
Observed strong gain dependence at 450 GeV and 4 TeV during Run 1!
LHC
M. Kuhn - Sept. 16, 2015
Photomultiplier Working Point at 6.5 TeV
o Measurements at 6.5 TeV more difficult.
− Smaller range of possible PM settings before ADC saturation.
o No evident sign of PM saturation at 6.5 TeV could be seen.
o Run 1 investigations showed significant dependency of measured beam size on PM settings.
LHC wire scanner upgrade during Long Shutdown 1:
− One broken wire scanner replaced (beam 2).
− Power supply schematics upgraded.
− PM gain dependency on light intensity reduced.
23
LHC
M. Kuhn - Sept. 16, 2015
LHC Optics Measurementso Can use results from optics measurements with the turn-by-turn
phase advance method and k-modulation for:
o Outstanding measurements:
− K-modulation at 6.5 TeV and after the squeeze
− Turn-by-turn phase advance measurements at 450 GeV (repeated) and during the ramp!
o For emittance plots: using measured b where possible
− b function measurement error < 3 %
− Maximum measured beta beat is 5 % at the wire scanners
− Linear interpolation during the ramp and squeeze
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IR4 IP1/2/5/8
Injection Ramp Flattop After Squeeze b*
K-modulation x xTurn-by-turn x x
LHC
M. Kuhn - Sept. 16, 2015
b* Measurementso Sinusoidal k-modulation in IP1/5 on August 8, 2015
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I = 10 Af = 0.01 Hz
Measurement error on tune oscillation amplitude in sub-percent level b* meas. uncertainty ≤ 1 % Beta beat ≤ 1 % Compatible with turn-by-
turn measurements
Preliminary!
IP1 [m] IP5 [m]
B1 B2 B1 B2b* H 0.81 0.79 0.80 0.80DbH 0.01 0.004 0.001 0.01b* V 0.81 0.79 0.79 0.79DbV 0.01 0.01 0.01 0.002
LHC
M. Kuhn - Sept. 16, 2015
Bunch Length Measuremento Longitudinal bunch shape not Gaussian at 6.5 TeV
− Due to controlled longitudinal RF blow-up at flattop energy
o But LHC bunch length monitor publishes 4s bunch length values based on FWHM algorithm assuming Gaussian profiles
Bunch length error ±1 cm!
“True” emittance from luminosity should be larger by 0.1 mm
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